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11
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On the slope of the scalar Kℓ3 decay form factor
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Renner, B.;
Wambach, U.M.;
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(Nuclear physics, B,
v.54,
1973,
pp.1-5)
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12
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Comparison of K<SUB>π3</SUB> experiments with predictions from equal-time commutators
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Nefkens, B.M.K.;
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(Physics letters,
v.22,
1966,
pp.94-96)
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13
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Matching chiral perturbation theory and the dispersive representation of the scalar <i>Kπ</i> form factor
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Bernard, Vé
ronique;
Passemar, Emilie;
Université
Louis Pasteur, Laboratoire de Physique Thé
orique, 3-5 rue de l'Université
, F-67084 Strasbourg, France;
Institute for Theoretical Physics, University of Bern, Sidlerstr. 5, CH-3012 Bern, Switzerland;
(Physics letters: B,
v.661,
2008,
pp.95-102)
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14
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Ballot permutations and odd order permutations
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Spiro, Sam;
;
(Discrete mathematics,
v.343,
2020,
pp.111869)
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15
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Local and unitary two particle saturation applied to K<sub>l3</sub> decay
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Gromes, D.;
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(Nuclear physics, B,
v.42,
1972,
pp.480-492)
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16
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Preparing for a decision support system.
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Callan, K;
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(Topics in health information management,
v.21,
2000,
pp.84-90)
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17
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RENORMALIZATION GROUP FLOWS IN NONPERTURBATIVE 2D QUANTUM GRAVITY
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FUCITO, F.;
MARTELLINI, M.;
CERN, 1211 Geneva 23, Switzerland;
Theoretical Physics, ETH-Hö
nggerberg, 8093 Zurich, Switzerland;
(International journal of modern physics. A, Particles and fields, gravitation, cosmology,
v.7,
1992,
pp.1361-1374)
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18
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Women's Running When faced with a mugger where was the fight or the flight?
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Callan, K.;
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(Runner's world,
v.12,
2004,
pp.51)
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19
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Robustness of the dispersive representation of Kπ form factors
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Oertel, M.;
;
(Nuclear physics. B, Proceedings, supplements,
v.186,
2009,
pp.330-333)
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20
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Computation of the running coupling in the SU(2) Yang-Mills theory
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Luscher, M.;
Sommer, R.;
Wolff, U.;
Weisz, P.;
;
(Nuclear physics, B,
v.389,
1993,
pp.247-264)